Sputtering coefficients in wall IDS #96
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These sputtering coefficients were introduced by the ticket IMAS-4287, for the needs of the DYON code (author: Hyun Tae Kim). |
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Ok, for the sputtering_physical coefficients the changes are clear. |
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Closed after the merge of PR #126 |
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The wall IDS contains a structure for sputtering coefficients, very well hidden under the name
global_quantities/neutral(i1)/incident_species(i2)
. It does provide for tabulation of the sputtering coefficients according to the incident species energy, but not the incident angle (while this can make a very large difference). The quantityglobal_quantities/neutral(i1)/incident_species(i2)/sputtering_physical_coefficient
has three dimensions, one of which is for the neutral type (1: cold, 2: thermal, 3: fast), which makes no sense to differentiate if we already have an energy dimension which separates the three populations and could instead be used for an angular dependence.I would request that an additional
global_quantities/neutral(i1)/incident_species(i2)/angles(:)
field be added to the structure, and the sputtering coefficients allowed to vary accorgin to the incident angle.Moreover, the naming convention for the three neutral types must always be understood WITH RESPECT TO THE PLASMA, and NOT the wall. This needs to be made more explicit in the documentation. "Thermal" neutrals are meant to be the ones which temperature has equilibrated with the main plasma ions, but in PWI parlance, would mean neutral emitted at the wall temperature, which in this IDS is referred to as "cold" neutrals. This confusion would be best avoided.
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